Abstract

We present a measurement of the Michel parameters of the $\tau$ lepton, $\bar{\eta}$ and $\xi\kappa$, in the radiative leptonic decay $\tau^- \rightarrow \ell^- \nu_{\tau} \bar{\nu}_{\ell} \gamma$ using 711~f$\mathrm{b}^{-1}$ of collision data collected with the Belle detector at the KEKB $e^+e^-$ collider. The Michel parameters are measured in an unbinned maximum likelihood fit to the kinematic distribution of $e^+e^-\rightarrow\tau^+\tau^-\rightarrow (\pi^+\pi^0 \bar{\nu}_\tau)(\ell^-\nu_{\tau}\bar{\nu}_{\ell}\gamma)$ $(\ell=e$ or $\mu)$. The measured values of the Michel parameters are $\bar{\eta} = -1.3 \pm 1.5 \pm 0.8$ and $\xi\kappa = 0.5 \pm 0.4 \pm 0.2$, where the first error is statistical and the second is systematic. This is the first measurement of these parameters. These results are consistent with the Standard Model predictions within their uncertainties and constrain the coupling constants of the generalized weak interaction.

Highlights

  • In the Standard Model (SM), there are three flavors of charged leptons: e, μ, and τ

  • The SM has proven to be the fundamental theory in describing the physics of particles; precision tests may reveal the presence of physics beyond the Standard Model (BSM)

  • According to Ref. [9], ξ κ is related to another Michel-like parameter ξ = −ξ − 4ξ κ + 8ξ δ/3

Read more

Summary

Introduction

In the Standard Model (SM), there are three flavors of charged leptons: e, μ, and τ. The SM has proven to be the fundamental theory in describing the physics of particles; precision tests may reveal the presence of physics beyond the Standard Model (BSM). I,j=L,R where GF is the chirality the Fermi indices of constant, i and the neutrinos, j are is e the chirality indices for the or μ, S = 1, V = γ μ, charged T =i γ leptons, μγ ν − γ n and νγ μ m √are /2 2 are, respectively, the scalar, vector, and tensor Lorentz structures in terms of the Dirac matrices γ μ, ui and vi are the four-component spinors of a particle and an antiparticle, respectively, and giNj are the corresponding dimensionless couplings. In the SM, τ − decays into ντ and a W −-boson, the latter (a) (b)

Objectives
Methods
Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.